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MODELING AND FINITE ELEMENT MASS TRANSPORT ANALYSIS OF A

POLYMER ELECTROLYTE MEMBRANE FUEL CELL AT DIFFERENT

OPERATING CONDITIONS

Bakiyalakshmi R.

1

, Deepti Suresh

2

and Vimala Juliet A.

3

1

Department of Instrumentation and Control Engineering, SRM University, Chennai, India 2

Department of Electronics and Control Engineering, SRM University, Chennai, India 3

Department of Instrumentation and Control Engineering, SRM University, Chennai, India E-Mail: deeptibinsur@gmail.com

ABSTRACT

In this investigation, a 3-D modeling of a PEM (polymer electrolyte membrane) fuel cell has been presented by considering Carbon nanotube (CNT) as the electrode and Cobalt as catalyst. Conventional fuel cells utilize graphite electrodes and platinum catalyst. Compared to mechanical and electrical properties of graphite, CNTs offer good mechanical strength and high current density. Similarly Cobalt has been considered as a cost effective counterpart to platinum. The simulation was carried out at 3 different operating temperatures (80oC, 120oCand 160oC) and the results were analyzed. The focus of this work is to design, analyze and compare the water concentration at the cathode side, using the above two catalysts.

Keywords:polymer electrolyte membrane fuel cell (PEMFC), GDL, CNT, modelling, catalyst, COMSOLTM.

Acronyms used

PEM Polymer Electrolyte Membrane LT Low Temperature

HT High Temperature GDL Gas Diffusion Layer CNT Carbon Nanotubes

INTRODUCTION

A fuel cell is a green electro-chemical device which converts the chemical energy of a fuel into electrical energy. The term green arises since it is a non-polluting power generator. There are several types of fuel cells which take in different fuels and generate electricity and give out useful by-products. For instance, from a Hydrogen fuel cell, we get a useful by-product water along with electrical output. A stack of such fuel cells can be combined to generate appreciable voltage. These fuels do not pollute the atmosphere with harmful greenhouse gases. A fuel cell has the following sections: Anode compartment, Cathode compartments each consisting of a Gas diffusion layer, Catalyst and an electrode. The two compartments are located separated by a membrane which acts as an electrolyte. The function of a GDL (Gas Diffusion Layer) is to enhance the reactant gas flow through the Membrane. The catalyst helps to speed up the reaction rate and in proton conduction. Anode and cathode electrodes are used for measuring the electrical output. The electrolyte plays a key role in the functioning of a fuel cell; it can be of solid or liquid form. In case of PEMFC the electrolyte is a micro porous membrane made of polymers as shown in Figure.

Figure-1. PEM Fuel Cell.

LITERATURE REVIEW

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the following work, analyzes the transport mechanism at three different temperatures using a cost effective catalyst.

FUNDAMENTAL LAWS ASSOCIATED WITH FUEL CELLS

The basic fuel cell reaction is Hydrogen oxidation reaction at the anode and reduction reaction at the cathode. The electrons after the generation of electricity combine with hydrogen ions that pass through the membrane and oxygen at the cathode and give out water as by-product.

Anode: 2 2−→ 4 ++ 4�− Cathode:4 ++ 4�−+ �2−→ 2 2

Darcy’s law

The Darcy’s law relates the velocity and viscosity of a fluid when it flows through a porous/permeable structure having small sized pores. It is given by

��

�� + ∇. �� = 0

Where

�: Density of the fluid

�: Dynamic viscosity

Brinkman’s equation

Since Darcy’s law deals with flow through micro pores and Stokes equation describes the flow through macro pores, pressure gradient at the boundary between the two regions is described by

P= -�/�*V+�*�*V Where

��: Effective viscosity in porous media

V: Velocity

K: Permeability of porous media

Tafel’s equation

The hydrogen reaction rate directly determines the current density of a fuel cell. When the current density is higher, there is a drop in the potential called as over potential. This drop is due to the resistance to flow of current at higher current densities. The following equation describes the relation between the over potential and the current density.

∆� = � ∗ � /

Where

A: Tafel’s constant

Io: Exchange current density (mA/cm2)

MODELLING SETUP

The structure consists of a detailed 3D volume based rebuilding of a HT PEM fuel cell. The structure consists of three compartments namely the Anode and Cathode compartments each consisting of electrodes,

Gas Diffusion Layer (GDL) and a catalyst layer. The electrodes are chosen to be Carbon Nano Tubes

(CNTs) and Catalyst is chosen to be Cobalt. Both the compartments are sandwiched on either side of a membrane which plays a vital role in generating a proton potential in the fuel cell. Each part of the fuel cell is built as separate block.

Assumptions

 The fluid used is incompressible.

 Pure oxygen is used at the cathode.

 The fuel cell operation is time-independent.

 Membrane is humidified completely.

 Flow is taken to be laminar.

MATERIALS

In order to have a proper understanding on the operation of a PEM fuel cell it is essential to rightly specify the materials for each of the layers in the cell. As the modeling involved was to optimize the design of a PEM fuel cell, to enhance the performance of it, choosing the best material was vital. Graphite Electrodes that were used previously as electrode material [7] were replaced by carbon nanotubes as they have really high strength and improved gas diffusivity, water drainage, and effective use of the catalyst [6]. Cobalt was chosen as a material of choice as it proved to be more stable than platinum and one of the major advantage is, it is of low-cost [12]. The material to be used for the membrane must be able to absorb some amount of the flowing reactants. Composite membranes are on a great interest due to their temperature tolerance compared to other materials [3].Polyamides are used as material for membrane which has high thermal conductivity. Graphite plates are used a gas diffusion layer material.

MODEL DEFINITION

A PEMFC model shown has been simulated using COMSOL MultiphysicsTM. The study was initially started with the conventional electrode and GDL and later changed to the proposed CNT and graphite. The following physics were included during simulation and the stationary study was done.

Figure-2. 2D view of simulated model of a PEM.

PHYSICS INVOLVED

Secondary current distribution

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Reacting flow through porous media-transport of concentrated species

The transport of concentrated species interface is used to study gaseous and liquid mixtures where the species concentrations are of the same order of magnitude and none of the species can be identified as a solvent. This physics interface includes models for multicomponent diffusion, where the diffusive driving force of each species depends on the mixture composition, temperature, and pressure. The physics interface solves for the mass fractions of all participating species.

Operating conditions

The analysis was performed at three different temperatures (80oC, 120oCand 160oC). The results were obtained for the mass transport of a fuel cell considering platinum as a catalyst as well as cobalt. A reference concentration of the reactants was given as 40.88mol/m3. The cell was operated at a pressure of 101KPa.The structure was mapped completely and swept with specific meshing size as shown in Figure-3. Stationary study was performed and the following results were obtained.

Figure-3. Structure after meshing.

RESULTS AND DISCUSSIONS

A single straight channel fuel cell operating at three different temperatures was studied with an operating cell voltage V_cell of 0.4V. This study was performed to compare the variations inthe amount of water concentration at the cathode side by using different catalyst. It has been observed that when operated at high temperature, the water concentration tends to reduce. Simulations were carried out using both the catalyst at same operating conditions as shown below.

Figures 4 and 5 indicate the water concentration at a temperature of 160oC for the catalyst platinum and cobalt respectively. Figures 6 and 7 present the molar concentration of water at a temperature of 120oC. Similarly Figures 8 and 9 compare the cathode water accumulation at a temperature of 80oC.It has been found that optimal performance of the fuel cell is affected if there is excess water in its stack. Hence water management is imperative in ensuring proper functioning of fuel cell.

Figure-4. Water concentration at the cathode using platinum at temperature of 160oC.

Figure-5. Water concentration at the cathode using cobalt catalyst .Simulations was carried out at operating

temperature of 160oC.

Figure-6. Molar concentration of water at the cathode side of fuel cell at an operating temperature of 120oC

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Figure-7. Molar concentration of water at the cathode using cobalt at a temperature of 120oC.

Figure-8. Cathode water concentration in the fuel cell at temperature of 80oC using platinum as a catalyst.

Figure-9. Surface Molar concentration of water at the cathode for a temperature of 80oC using cobalt.

CONCLUSIONS

In this study, a detailed model of a straight channel fuel cell has been presented. The proposed model considers the water accumulation at the cathode side due to the redox reaction inside the fuel cell. Different catalyst has been considered in this study. The results indicated that performance was unaffected even after replacing the catalyst and the membrane by the proposed cost effective material. Further investigations are in progress to investigate electrochemical behavior of the fuel cell when subjected to similar operating conditions.

REFERENCES

[1] Jie Peng, Seung Jae Lee. 2006. Numerical simulation of proton exchange membrane fuel cells at high operating temperature. Journal of Power sources. Vol. 162(2): 1182-1191.

[2] D. Maillet. 2007. Modelling of heat, mass and charge transfer in a PEMFC single cell-Journal of Power Sources. Vol. 145(2): 416-427.

[3] Pera M.C. 2007. Power Generation of Fuel cells- Industrial Electronics Magazine, IEEE. Vol. 1(3):34-35.

[4] Fei Gao, Student Member, IEEE, Benjamin Blunier, Member, IEEE, Abdellatif Miraoui, Senior Member, IEEE, and Abdellah El Moudni. 2010. A Multiphysics Dynamic 1-D Model of a Proton-Exchange-Membrane Fuel-Cell Stack for Real-Time Simulation IEEE. Vol. 57(6): 1853-1864.

[5] Park Jong, Branko N, Popov. 2012. A review of gas diffusion layer in PEM fuel cells: Materials and designs- International Journal of Hydrogen Energy. Vol. 37 (7): 5850-5865.

[6] Amrit Chandana, Marisk Hattenbergera, Ahmad El-kharoufa, Shang Feng Dua, Aman Dhira, Self, Bruno G. Polletc, Andrew Ingrama, Waldemar Bujalskia. 2013. High temperature (HT) polymer electrolyte membrane fuel cells (PEMFC). A review- Journal of Power Sources. Vol. 231(1): 264-278.

[7] Benoit Bidoggia. 2013. Estimation of Membrane Hydration Status for Standby Proton Exchange Membrane Fuel Cell Systems by Impedance Measurement: First Results on Variable Temperature Stack Characterization-International Journal of Hydrogen Energy. Vol. 38(10): 4054-4056.

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proton exchange membrane fuel cells-Journal of Power Sources. Vol. 253: 104-113.

[9] C. Sterniga, C. Finkb, V. Hackera, A. Theilera, R. Tatschl. 2015. Theoretical study of the influence of material parameters on the performance of a polymer electrolyte fuel cell- Journal of Power Sources. Vol. 297: 329-343.

[10]Andreas Theiler, Larisa, Karpenko-Jereb. 2015. Modelling of the mechanical durability of constrained Nafion Membrane under humidity cycling- International Journal of hydrogen energy. Vol. 40, (31):9773-9782.

[11]Rasol Abdullah Mirzaie, Fatemeh Hamedi. 2015. Investigating New Electro catalyst for Polymer Electrolyte Membrane Fuel Cells and the Effect of Carbon Additives in the Reaction-Indian Journal of Science and Technology. Vol. 8(11), 70727.

[12]Nagai M, Sanpei H, Shira Kura M.J. 2012. Cobalt porphyrin-tungstenpolyoxometalate anion as non-noble metal cathode catalyst in a fuel cell- Material Chemicals. Vol. 22(18): 9222-9229.

[13]R. Taccani et al. 2011. Power Generation of fuel cells-International Journal of Hydrogen Energy. 36(16): 10282-10287.

[14]N.A. Karim, S.K. Kamarudin. 2013. An overview on non-platinum cathode catalysts for direct methanol fuel cell, Applied Energy. 2013, vol. 103: 212-220.

References

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